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18:00
I may be able to turn it inside out to fix it, but if I'd have to re-tape it I won't bother
Or just pretend you meant to do -log from the beginning.
post a snapshot
I will, after I redo it. Messed it up while trying to fix that
ping me with it when you're done
18:04
It's for the Lambert W function btw
ah. don't think i remember how it looks, all the more reasons i need a snapshot
Yeah
To see why it's weird, see the presentation of branch points here: functions.wolfram.com/ElementaryFunctions/ProductLog2/04/04/01
You can also find the discussion of branch cuts nearby on that site
How do I solve this: (x^2 - 9)/(3x - x^2 - 24) < 0 ?
Cry
Alternatively factor both numerator and denominator and draw where the numerator and denominator are positive and negative
18:20
lol
Ok, here's my attempt to take a pcture
That's intended as branches -1,0,1 from bottom to top
Cool model
If I wind around the edge of the three surfaces, I'll go -1 to 0 to 1
But I can also go directly from branch -1 to 1
That's the piece of paper which lies between the pair of double arrow
18:31
Ah
Both of which are on the 0 branch. (The arrows are to remind me that said piece of paper doesn't stop me from moving from one side of the 0 branch to the other (the branch cut on this surface starts at -1/e.)
Right, I understood that. It lives as an embedded surface in C^2
That means that the branch point at -1/e is of order 2.
so if I start to the right of -1/e on the 0 branch and make two revolutions around that point, I'll go 0 to -1 to 1 to 0
Which is kinda goofy!
The Lambert W function has caused me nothing but confusion. This is no different.
that's about how I feel tbh
But this may be enough to do what I want.
Namely, there's a difference between this and the log case. There, the difference between log(z) above/below the cut is $2\pi i n$ depending on which branches of log i compare
So if I start at a point on one branch and analytically continue to the same point on another branch, I only have to worry about the winding number
That's not true in the Lambert W case, since I can wind around the -1/e branch either once or zero times
Hence there's an additional ambiguity for analytic continuation, and that's exactly what I want
( I guess I'm going from $\pi_1=\mathbb{Z}$ to $\mathbb{Z}\times \mathbb{Z}_2$)
19:19
Shot in the dark here, but: Anyone on that happens to be familiar with writing things to a CSV file, in Python? I have a list of 6,240 "objects" that took a couple hours to generate, and are going to vanish unless I figure out how to record them somewhere...
19:49
Downgrade to threat level orange: data appears safely recorded.
20:30
haha
glad to hear you figured it out man
21:09
Is there an official mathematical definition of "spiral"
that includes logarithmic spirals and helices
Do you want the definition to include all kinds of spirals, or is it fine if it mostly covers just those two?
I came up with a sort of "joke" the other day...
What does $\int d^n x$ mean?
Mathematics is purely a figment of our imagination; it is not a part of reality. It is, however, a conservative extension of reality.
Does it mean integrating a differential of $n$ components?
Meaning, whenever mathematics proves something about reality, it's true in reality?
21:20
Hello!
@AkivaWeinberger Yeah.
Actually, I have a better phrasing. Mathematics is all made-up; it's not really true. It is, however, a conservative extension of the truth.
21:36
Anyone here knows the meaning of "normal trajectory of a surface"? (from Differential Geometry)
22:33
@TedShifrin @Astyx @LeGrandDODOM A propos de l'endroit exact où se retrouver, je propose le parvis de l'église Notre-Dame-des-Champs
22:50
Ça me va
@Astyx On se fixe un horaire ? 12h30 par exemple ?
Hey everyone!
@TedShifrin you're back! If only for a bit
Heya @Semi
Why is it that $\mathcal{B}^{2n}_r(P)$ approaches a square as $n$ increases? This is in $\mathbb{R}^2$
I.e., why does the set of points $\{(x,y) : (x^{2n}+y^{2n})^{1/2n} < r \}$ describe an open "square" as $n \to \infty$?
Thanks!
Do you see why, @Semiclassical?
23:10
1) you can focus on the case of $r=1$ since you could change coordinates to $u=x/r$, $v=y/r$ and get $u^{2n}+v^{2n}=1$.
Sure
2) The curve has 8-fold symmetry (symmetric across the axes and upon exchange of y=x), so it's enough to focus on arc where $0<x<y<1$.
Hmmm
8-fold symmetry?
Sure. It's symmetric w/r/t $x\to -x$ so it's got a reflection symmetry across the y-axis.
Similarly w/r/t $y\to -y$.
Finally, it's also symmetric if we swap $x,y$ (i.e. reflection across the line $y=x$.)
(Those in turn generate a further symmetry across the line $y=-x$.)
Ah, yes that makes sense
23:16
mmkay
Now, note that $x<y$. Hence as $n\to \infty$ it'll be the case that $x^{2n}\ll y^{2n}$.
So for large $n$ it should be the case that $1=x^{2n}+y^{2n}\sim y^{2n}$.
So $y\to 1$ and $x\to 0$.
Ahh so we get a line
Right.
Now, that's possibly a bit handwavey.
To do it right, one should probably solve for $y$ in terms of $x$, subject to $0<x<y<1$ since we're in the first octant as I indicated earlier, and show that $y\to 1$ as $n\to \infty$.
Incidentally, this idea shows up outside of geometry: In the realm of analysis, it's the basis of the uniform norm aka sup norm aka $\infty$-norm.
It means that the sup norm is a limiting case of a p-norm.
(Similarly for the inf norm)
Is it obvious where the line(segment) has its start- and endpoint?
Well, when $(x,y)=(1,0)$ one always has $x^{2n}+y^{2n}=1$.
So that's always a point on the curve.
Similarly, when $x=y$ you've got $x^{2n}+y^{2n}=2x^{2n}=1\implies x=y=2^{-1/2n}\to 1$ as $n\to \infty$.
So the curve will have $(x,y)=(1,1)$ as a point as well.
From there, symmetry does the rest.
Okay, out for now.
I mean on the arc
Alright, thanks for the help :)

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